Oscillation generation system



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Patented May 18, 1954 UNITED STATES PATENT OFFICE OSCILLATION GENERATION SYSTEM Roger Bataille, Montmorency,

and Georges Honorat, Neuilly-sur-Seine, Seine, France, assignors to Societe Franaise des Telecommunications, Neuilly-sur-Seine, Seine, France, a corporation of France Section 1, Public Law 690, August 8, 1946 Patent expires November 23, 1962 (Cl. Z50- 36) 14 Claims.

Many attempts have been made by those skilled in the art to stabilize radio-electric transmitters and receivers in order that for any well determined position of their controls, they will be tuned on a well determined constant wave length. In the devices of the conventional type, the desired frequency variations in transmission as well as in reception are obtained by means of at least one variable capacitor. Under the effect of a number of factors, such as variations in temperature, pressure, etc. the resonance frequency may vary in the conventional devices, for the same position of the controlling member, by about 1/1000; therefore, frequencies higher than 50 lic., this variation may escape the tuned band of a receiver initially suitably adjusted. This is the reason why it has been necessary until now to tune up the receiver, i. e. to use a trial and error method acoustically appreciating the changes in intensity of the reception, and even, in certain cases, to alter the adjustment of the receiver during the reception.

Attempts have already been made to eliminate this defect by using crystal devices to determine the resonance frequency of a transmitter or of a receiver. Quartz or piezo-electric crystals do indeed enable the determination of the frequency with a much higher precision of the order of l/100,000. However, these devices have not so far allowed a continuous variation. A quartz device gives. only, for example, the basic frequency and its various harmonics, i. e. in any case a strictly limited number of frequencies. Practically, this results in a number of defects, particularly in the military field, where the resultant necessity of transmitting over one or more determined frequencies of limited number allows easy identification of the transmitter using said frequencies.

The present invention has for its object to benefit simultaneously from the advantages inherent to oscillating devices of the quartz type and to oscillators of the continuous type, eliminating simultaneously the defects of each of these devices. According to the invention, the frequency band on which it is desired to operate continuously, and which may be a very large one, as a matter of fact a band covering all frequencies used in radio-electric transmissions, is covered by one r more quartz devices, preferably not more than one or two, which, taking into account the crystal or crystals harmonics, divides the said band into elementary bands, which bands may be covered continuously by means of an oscillator of a known continuously variable type. In other words, if it is desired to tune a transmitter according to the invenfi O tion on any wave length which the set uses, the set is tuned by means of a quartz device on an approximate frequency supplied by the piezoelectric oscillations, the negative or positive complement to obtain the desired wave length being supplied by the continuously variable oscillator.

This application is a division of application Serial No. '104,074 filed October 18, 1946, now Patent No. 2,606,285, for Double Heterodyne Radio Receiver.

In a transmitter accordingr to the invention, oscillationsl supplied by a continuously variable frequency oscillator of low frequency, having accordingly only a small drift, are mixed with oscillations supplied by one or more oscillating devices, the frequency of which is stabilized by a piezo-electric crystal either on the value of the resonance frequency of the crystal, or on one of its harmonics, the frequency value of the continuously variable oscillator, the value of the resonance frequency of the crystal or crystals and their harmonics and the mixture of said component oscillations being such that the frequency of the resulting oscillations may have any desired value over a continuous band of frequencies, the width thereof being practically as large as desired.

It will be seen, on the one hand, that the whole of the band may be covered in a continuous manner as in the case of an oscillator of the conventional type and, on the other hand, that the maximum error introduced, which is obviously the sum of the errors introduced by the quartz device and by the continuous variation oscillator, is always very small. The error resulting from the quartz device, amounting to only 1/100000 of its frequency, always remains very small even if said frequency is high; the error introduced by the continuous variation oscillator, though amounting to 1/1000 of its frequency, is small, as this frequency has a small absolute value, amounting only to the complement to be added to the frequency supplied by the quartz device.

If it is desired, for example, to accurately and continuously cover a band from 0 (theoretical) to 30,000 kc. or more, in practice from kc. to 30,000 kc., the following method may be used: a first quartz stabilized oscillator provides with a single crystal frequencies of 1000, 2000 etc. up to 30,000 kc. which differ vone from the other by 1000 kc. A second oscillator, again quartz stabilized, provides with a single crystal, in each of the 1000 kc. sections thus defined, intermediate divisions having 100, 200, v300 etc. up to 1000 kc. difference. A third oscillator continuously variable from` 1 0()4 to200 kc., consisting of an oscillator of the conventional type, provides a continuous variation in each of the 100 kc. bands thus limited.

The maximum errors thus introducedare as follows: in the first quartz circuit: 0.30 kc.; in the second quartz circuit:-;01^;kc.; inthe continuous variation circuit: 0.2.kc.; i. e. a totalof 0.51 kc. Said maximum variation will not tune cut of the passing band of a receiver so that this latter keeps tuned inspite. of all disturb.-

it will be sucient to adjust-the controls of the receiver in the position corresponding to said wave length, without hunting oriacoustic appre..

ciation.

On the other hand, the resulting frequency has no troublesome parasiticfrequencies, the nearest one being -30 decibels, far from the useful final tone in even the most unfavorable case.

Inthe above example, the control operations for-reception are limited to three:

(l) i Selection of thethousandsfof kc. by means of a 30 step` switch (2) Selection of the hundreds of kc. by means ofa l0 step switch;

(3) Selection of theiiunitsfrom 0 to 100 kc. by means-of a graduated-dial.

In the form of execution of a transmitter according to the p resent invention, to the oscillations generated bythe low` frequencies oscillator able to-varyin a continuous manner, there will be added fixed frequency oscillations, generated for example byoneof the piezo-electric stabilized oscillators,- before mixing them with the component oscillations generated by the other crystal oscillator or. oscillators.

This previous addition, raising the value of the frequencyA of the oscillations varying in a continuous manner in frequency, makes easier the selectionof the resulting oscillations.'

The vfixed. frequency oscillations may-be added to the oscillations from the continuously variable oscillator by using Aa symmetrical system. This will allow the eliminatiorrof Lthe harmonics of the continuously Variable oscillationsv which, otherwise, might lead to interferences for certain frequency values.

In the above numerical example, the elementary interval ofthe rst harmonic scale is 100 kc'. and the elementary interval of the other harmonicv scale is 1000,kc. Two piezo-electric crystals are used for these harmonic scales.

In an alternative embodiment, only lone piezoelectric crystal is used for both'scales, the one being obtainedin the manner above described, i. e. from a,stabilizedwoscillator with a, piezoelectric crystal, andthe. other one by means of an oscillator the frequency stability. of which will be obtained through synchronization from the first oscillator. Thus one crystal only is necessary.

In one form of execution of the invention, the continuously-ya1iable oscillations are mixed in thenrst instance 4,with theharmonics of the lowest scale.

On the contrary, inan alternative embodiment the oscillations from Y the low frequency oscillater,l the `frequency of which may Vary in a continuous mannen, ,are lpreviously. mixed with the oscillations of the highest scale of harmonics. The resulting oscillations4 are A thusdisposed in distant enough sections ofthe frequency spectrurn` anditl isV thus unnecessary for, theirr selec-.-

tion` to use devices comprising Variable condensers, eliminating thus the problem-of ganging them.

In the following description, reference is made f to the annexed drawings, in which:

Figure l is a block diagram of a transmitter according to the invention;

Figure 2 is a block diagram of a transmitter according to the invention, for another embodiment;

Figure 3 shows diagrammatically an embodiment of the control means for the embodiment of Figure 2;

Figure 4 is awning diagram for the embodiment of Figure 2;

Figure 5 is a block diagram of another embodiment;

Figure 6 is a block diagram of another embodiment;

Figure 7 is a block diagram or" a specific variation ofthe block diagram shown in Figure 6;

Figure 8 is a block diagram of another embodiment;

Figure9 is a block diagram of another embodiment;

Figure l0 is a block diagram of another embodiment;

Figure 1l is a wiring diagram of the embodiment shown on FigurelO.

It is pointed out that inthe following description, the numerical examples given for the frequency values are `intended only for a proper understanding oi' the description.

Reference will first be made to Fig. l. In the exemplary embodiment shown, a transmitter according to our invention comprises a piezo-electric crystal oscillator a supplying frequency-stable oscillations at a frequency equal to the fundamental frequency of the crystal. This oscillator is followed by a harmonics generator ZJ which supplies output oscillations at a plurality or succession4 of frequencies or harmonics of the said fundamental` frequency. The harmonics generator b is followed by a harmonic selector c which suppliesan output which comprises only a single one of the harmonics of the said multiplicity of harmonics fed to it,. the order of this harmonic being defined by the settingof a selector member d adapted to connect into the circuit a desired one of a plurality of oscillating circuits. The harmonic selected by the selector c is mixed, in a mixer e, with oscillations having a low natural. frequency supplied by an oscillator f, the frequency of which being continuously variable within an interval substantially equal to that between two successive ones of said harmonics. The frequency of the oscillations supplied by the oscillator f is dependent on the setting of la variable condenser g. The resultant s oscillations from the mixing step at the output from mixer e Vare fed to a lter h,4 the passing frequency. of which is controlled by means of a step-by-stepA operable selector member i and a Variable condenser j. k'isprovided betweenthe movable parts of both condensers g and j which are thus operable from a common control member Z. A further mechanical connection m is provided between the selector members d and z' which are thus operable from a common control button n.

Assuming itis desired to tune the transmitter thus described to any desired wavelength of a continuousfrequency band, the harmonic selector d lis,.through actuation of the button n, so,

A mechanical connection.

approximating in frequency the desired frequency, and the continuously-adjustable oscillator f is, by means of the member l, adjusted to the frequency value which is the positive or negative complement of the said harmonic in order to obtain the desired frequency; e

Rather than a single piezo-electric crystal-controlled oscillator, two crystal oscillators may be used. In such an embodiment of the invention,

there may be combined, with a conventional continuously-variable oscillator of any suitable type, a first crystal oscillator adapted to be adjusted to any one of a number of predetermined frequencies, i. e. the fundamental crystal frequency and a number of the harmonics thereof, and a second crystal oscillator adapted to be adjusted to any one of a number of predetermined frequencies i. e. the fundamental frequency of the second crystal and a number of its harmonics.

If, for example, it is desired to cover with the device according to the invention, in a continuous manner, the frequency band between 100 kc. and 30,000 kc., the oscillators may be selected with characteristics such that the oscillator A will generate oscillations capable of continuously varying from 100 kc. to 200 kc, the oscillator B generating frequencies of 100, 200, 300, etc. up to 1000 kc., the oscillator C generating oscillations of a frequency of 1000, 2000, 3000 etc. up to 30,000 kc. lf, for example, it is desired to tune the set on the 24,495 lac. frequency, the oscillator C will be adjusted on 24,000 kc., the oscillator B on 400 kc. and the oscillator A on 95 kc.; these frequencies are added and the final frequency is the desired frequency. Said frequency is obtained with an error of 0.5 kc. at the most, as stated above.

Referring now to Fig. 2 showing a simplified diagram of an oscillation generator executed in accordance with the invention, said device includes an oscillating device l, of the continuously varying conventional type, which may gencrate oscillations of a frequency Fi capable of varying in a continuous manner, for example from 100 to 200 kc. An oscillator 2 of the piezoelectric quartz type having a resonance basic frequency of 100 kc. may generate by using ten harmonics, oscillations of a frequency F2 differing one from the other by 100 kc., namely 900, 1000 etc. up to 1800 kc. The Fl and F2 oscillations are each fed to a mixer 3 of conventional form, from which issue after mixing the oscil lations Fl, F2 and F3, the latter being the sum of the frequencies of the incident oscillations. llhe output of mixer 3 is fed to a lter l which being adjusted according to oscillators l and 2, eliminates the Fl and F2 oscillations, passing oscillations F3 alone.

A second piezo-electric oscillator 5, the quartz of which has a resonance basic frequency of 1000 kc. for example, gives, by means of its harmonics, oscillations F4, having a 1000 kc. difference and which have as desired a frequency of 2000, 3000, etc. up to 10,000 kc. The F3 and F4 oscillations are each fed to a mixer 0, from which issue the oscillations F3, the oscillations F0 and oscillations F5, the frequency of the latter being the sum of the F3 and F4 oscillations.

Mixer S is followed by a filter 'l filtering by 1000 kc. steps, from which issue only the F5 oscillations but not the and F4 oscillations.

The oscillations Fi being capable of varying in a continuous manner from 100 to 200 irc. and the oscillations F2 varying per 100 kc. steps, from 900 to 1800 kc., the oscillations F3 may vary in 6 a continuous manner from i000 to 2000 kc.; the oscillations F4 varying per 1000 kc. steps from 2000 to 10,000 kc. the oscillations F5 may vary in a continuous manner from 3000 to 12,000 kc.

The least favorable case in regard to filtering in lter 'i will take place when the latter receives oscillations Fd having a 10,000 kc. frequency and oscillations F5 having a frequency of 11,000 kc. Nevertheless ltering will be easily performed by means of a standard filter, the selectivity curve of which allows a tuning up to two decibels for a passing band of 100 kc. and affords a 30- decibels -rdifference between the center of said band, corresponding to a frequency of 11,050 kc. and the nearest frequency, i. e. 10,000 kc. In practice the elimination of the oscillations F4 of a frequency equal to 10,000 lic., in the most unfavorable case, will be total and will be obtained by means of a filter of a standard type.

The filter l is followed by a separator-anddoubler device 0 which comprises three oscillating circuits 0', 0, 0', adapted to pass, respectively, the first, oscillations from 3,000 to 6,000 kc., the second, oscillations from 6,000 to 12,000 kc. and the third, oscillations from 12,000 to 24,000 kc., the output oscillations being then.I radiated from the antenna, after rst being inod-l ulated by an audio-frequency modulator.

Referring now to Fig. 3, certain characteristics of the mechanical switches of an oscillation generator constructed for a receiver according to the invention will be described. The continuously variable oscillator l includes for tuning purposes a @variable condenser 0 controlled by means of a knob l0 and a suitable mechanical transmission il.

The piezo-electric oscillator 2, generating oscillations varying from 000 to 1800 kc. per 100 kc. steps includes a control lever or similar member l2, having ten steps according to the ten frequencies it may generate and is controlled by a ten step knob i3 and a suitable gearing I4.

Filter 0 comprises two tuning members, namely a variable condenser l5 fitted on gearing li, the

capacity of which varies in a manner corresponding to variable condenser 0 conventional arrangements are used to gang the circuits, the second controlling member of filter 4 having a lever l0 to insert in the circuit suitable inductances if; said lever fitted on gearing i4 operated in turn by knob i3 inserts in filter Li,l00 lac.V stepped variations in a similar manner to the oscillator 2.

The frequency of the piezo-electric oscillator 5 is controlled by a ten step lever l0 to obtain frequencies from 2000 to 10,000 kc. per 1000 kc. steps. Lever i3 is operated by means of a knob i9 and a gearing 20.

Filter l comprises two controlling members, namely a first lever 2i fitted on gearing is, cooperating with inductances 22, and a second lever 23 fitted on gearing 20 and cooperating with inductances 24. The set of levers 2l and 23 permits the adjustment of the nlter on frequencies comprised between 3000 and 12,000 irc., with an interval of 100 kc. between them.

Knob l0, the units knob, capable of being moved continuously, has for example a mark moved before a lic. scale graduated from 0 to 90. The 10 step button i3, or hundreds knob, has a mark moving before a scale graduated from 0 to 9. Button I9, the thousands button, has a mark moving before a scale graduated as follows: 3, 4, 5 etc. up to 11.

Under suchrconditions, to adjust the transmis- 'sion on a determined frequency, knobs i9, i3 and |0.will be adjusted to the corresponding figures, respectively to the figure of thousands, the figure of hundreds and the number of units, from 0 to 100, of the desired frequency. For example to adjust the transmissionon a frequency of li583 kc., knob l0 will be brought opposite digit 4, knob I3 opposite digit 5 and knob l0 opposite the division 83.

The quartz oscillators include known means to produce an output having a constant amplitude to 1 decibel for any order of the harmonic used.

Fig. 4 is a wiring schematic given by way of example ofk a preferred embodiment of a trans mitter according to the invention, the frequency of Which may Vary in a continuous manner, for example from 3000 to 12,000 kc. Said device includes a pentode tube oscillator LI, generating harmonics, excited by means of a quartz crystal QI having a basic frequency of 100 kc., an oscillating circuit comprising the inductance Si and the capacitor Ci, and tuned to said frequency. The grid leak of tube Li is RI and the drop resistance of the screen grid of said tube is C2 is a capacitor for uncoupling the screen. The oscillating circuit F2 fitted to the output of rtube L! comprises a fixed capacitor C3, and a ten tap inductance S2 to tune the circuit as desired on 900, 1000, 1100 etc. up to 1800 kc.

rllube L2 is a self-excited triode, the oscillating circuit Fl of which comprises an inductance S3 and a capacitor C0 consisting of a variable condenser in order that the oscillations from said tube L2 may vary in a continuous manner from 100 to 200 kc. C5 is a coupling capacitor and R3 is the grid leak.

The oscillations from pentode tube Ll and triode tube L2 excite the tube L3 of a first frequency changer, respectively through a coupling capacitor C0 of the injection grid and a coupling capacitor Cl of the control grid. Rf: is the control grid leak and Rthe injection grid leak, C8 the screen uncoupling capacitor, R0 the drop resistance of the screen.

A lter oscillating circuit Flcomprises a ten tap inductance Sd the lever of which is mechanically coupled to the lever of inductance S2, for simultaneous operation; the capacity of the oscillating circuit F3 is constitutedby a variable condenser C0 which, through a mechanical coupling, has a homologous position with `condenser C4. Capacities are series-connected to the various taps of winding S0 in order to gang the circuits by known means. The oscillationsrfrom the first frequency changer are the resultof the addition of the oscillations from the pentodel tube L! and the triode tube i2, excluding theoscillations proper to said tubes; accordingly they may vary in a continuous manner from 1000 to 2000 kc.

A second oscillator and harmonic generator pentode tube L4 includes in its oscillating grid circuit a crystal Q2 having a resonance basic frequency of 1000 kc. for example; R? is an oscillating grid leak and R0 a drop resistance of the screen grid. The oscillating circuit of tube Le includes an inductance S5 and a capacitor Cl adjusted to a 1000 kc. frequency. CII is an uncoupling capacitor for the screen grid. The outlet of tube L0 includes an harmonic lter circuit F4, consisting in a nine tap inductance S6 and a condenser CI2 which may be tlius tuned on v2000, 30004000, etc. up to 10,0002 kc.

The oscillations from the pentode tube Lil and those from the first frequency changerare simulpass through a filter 208.

taneously fed to a tube L5 of a second frequency changer, the rstfones through a capacitor CIS coupling the control grid and the second ones through a capacitor CIS coupling the injection grid. R9 is a control grid leak and Rit an in- `iection grid leak. Cll is a capacitor for disconnecting the screen grids.

r'he outlet of the second frequency changer includes an outlet lter circuit F5 consisting in a. ten tap inductance S1, the hand lever of which is mechanically' coupled to hand levers of in-v ductances S2 and gSfl. The lter circuit F5 ina cludes further a nine tap inductance Si', the hand lever of which is mechanically coupled to the hand lever of inductance S5. Cil! are fixed capacitors which may be selectively inserted into the circuit, corresponding to the nine positions of the hand lever of inductance Sl.

Oscillations from the described device are fed to the following stages through the coupling-capacitor Cl5, and may have at Will any value between 3000 and 12,000 kc. in the selected example.

The apparatus diagrammatically illustrated in Fig. 5 makes it possible to cover in a continuous manner a frequency band extending from theoretical zero to 30,000 kc., or in practice from say 100 kc. to 30,000 kc. A first oscillator 20l is controlled by a crystal having a fundamental frequency of 1000 kc. This is followed by a harmonics generator 202 followed-n turn by a harmonic selector 203 which thus supplies output oscillations at any one of the frequency succession 1000, 2000, etc. up to 30,000 kc. The apparatus includes a second oscillator 200 stabilized f by a quartz crystal having the fundamental frequency 100 kc., and followed by a harmonics generator 205 followed in its turn by a harmonic selector 200. In mixing, in a mixer 20?, successively the harmonics issuing from selector 205 withV a harmonic issuing from the selector 203, each of the 1000 kc. sections defined by the selector 203 is divided into intermediate subdivisions of 100, 200, 300, etc. up to 1000 kc. The resulting oscillations at the output from mixer 201 The apparatus further includes a third oscillator 200, continuously Variable in frequency over a range of from 100 to 200 kc. The oscillations issuing from the oscillator 209, which thus enable a continuous variation over any one of the intermediate 100 kc. bands thus defined, are mixed with the oscillations from the filter 200 in a mixer 2 l0, and the resulting oscillations, after first having been passed through a filter 2H, radiated by an antenna 212.

In the embodimentillustrated in Fig. 6, the oscillations issuing froman oscillator 220, continuously-variable in frequency, are passed through a tunable circuit 22|, mixed in a mixer 223v with fixed frequency oscillations issuing from a crystal-stabilized oscillator 220 including a tuned circuit 225, so that the resultant oscillations may easily be filteredl in a filter 22S. The resultant oscillations are mixedv in a second mixer 221 with oscillations issuing from an oscillator 228 controlled by a crystal 229 and including a tuned circuit 230. The oscillator 228 is followed by a harmonics generator 23| followed in turn by a. harmonic selector 232. The oscillations provided by the mixer 221 next pass through a filter 233 adapted to pass only the resultant oscillations.

The form of embodiment shown in Fig. '7 is similar to the foregoing, except that a single oscillator'f 230 herein fulfills the functions of the oscillators 224 and 228 previously mentioned.

The oscillator 234 controlled by crystal 235 and including a tuned circuit 236 directly feeds fixed frequency oscillations to mixer 223. The oscillations fed to the second mixer 221 also come from the oscillator 23d provided with the tuned circuit '232, but through a harmonics generator 23? followed by a harmonic selector 238.

In the embodiment of Fig. 8, a single piezoelectric crystal is used for obtaining both successions of harmonics. rf'he oscillator 200 is controlled by a crystal 239 whose fundamental frequency is 1000 kc. Following oscillator 240 is a harmonics generator 2M, followed by a harmonic selector 242. The selected harmonic is mixed in a mixer 243 with the oscillations from an oscillator 204 continuously adjustable in frequency over a 100 kc. interval, the resulting oscillations being passed through a lter 245. The oscillator 246 provided for supplying a second succession of harmonics is, in this embodiment, frequencystabilized from oscillations derived from the first oscillator 240. The stabilized oscillator 240 is followed by a harmonics generator 201 followed in turn by a harmonics selector 240. The selected harmonic from the second succession is mixed in a second mixer 240 with the resultant oscillations fed out of the lter 245, and the oscillations issuing from this mixing are after being passed through a filter 250 which only passes the resultant oscillations, fed to the output circuit.

In the embodiment of Fig. 9, the higher-frequency harmonics succession is supplied by a crystal-controlled oscillator 260 followed by a harmonics generator 26I anda harmonic selector 262. The selected harmonic is mixed in a rst mixer 263 with oscillations from a continuously frequency adjustable oscillator 201i. The

oscillations resulting from the mixing may easily be separated in a filter 265 which it is not necessary to provide with variable condensers, thus eliminating the problem of their gauging, as their frequencies differ greatly from those of the component oscillations. The said resultant oscillations are mixed in a second mixer 260 with one harmonic of the lower-frequency succession of harmonics supplied by a crystal oscillator 261 followed by a harmonics generator 268 followed in turn by a harmonic selector 203. The oscillations issuing from this second mixing are passed through a filter 210 adapted to pass only the resultant oscillations, and are fed to the output circuit.

Referring now to Fig. 10 showing a block diagram of an alternative form of the device, the latter includes an oscillator 5I, whose frequency FIG! may be varied in a continuous manner, for example between 200 and 300 kc. Said oscillator includes an oscillating circuit 52. A second oscillator 53, whose frequency is controlled by a piezo-electric crystal 5d and includes an oscillating circuit 55, supplies at its outlet oscillations of a'xed frequency Fi l, for example 1000 kc.

The oscillations of frequency Fi@ are added to oscillations of frequency FII. Said addition is preferably achieved in a symmetrical device and the resulting oscillations, without the component oscillations eliminated in filter 5l, have a value of PE2 which, in this instance, may vary in a continuous manner between 1200 and 1300 lo.

The oscillations of frequency FII excite an l.

added in a mixer 00 to the oscillations of frequency FI2.

Iii

In the example shown, the devices 58 and 59 supply the harmonics of 6th to 10th order of the resonance frequency of crystal 54, i. e. oscillations of 6000, 7000 etc. up to 10,0-00 kc.

The set includes a third oscillator 6I, whose frequency is stabilized, not by a piezo-electric crystal being part of this oscillator, but through synchronization from the rst crystal oscillator 53. Oscillator 6I supplies oscillations of fixed basic frequency, for example of 100 kc., at a value determined by an oscillating circuit 62, and feeds an harmonics selector 63--64 in order to obtain the harmonic of the selected order. In the example shown, thus, harmonics of the 6th to 17th order of the basic frequency of the oscillator 6I may be obtained and the oscillations from filter @il have as desired a frequency FI4 equal to 800, 900 etc. up to 1700 kc.

The oscillations, of frequency FI5, resulting from mixing in device the oscillations of frequency FIS and FIZ and selection in filter are mixed in mixer 66 with the oscillations of frequency FHI and the resulting oscillations, of frequency Fl, after elimination of the component oscillations in lter 6l, are led to the conventional amplification stages of a transmitting set. I

Fig. ll is a wiring schematic of one form of execution of such a device.

The oscillations whose frequency may vary in a continuous manner, for example from 200 to 300 kc., are generated in an oscillating tube I0 composed of the usual parts, the oscillating circuit ll including a variable condenser 'I2 to adjust the frequency of the oscillations to any selected value between 200 and 300 kc.

Said oscillations are led in parallel to both injection grids 'i3 and 'I4 of tubes I5 and 'I6 excited on the other hand in'opposition by their grids 'i8 and 'i9 with the oscillations of xed frequency,

for example 1000 ko., generated by an oscillating tube B0, whose frequency is stabilized by a piezoelectric crystal 2|; said oscillations are taken'at the ends of the secondary winding 32 of a transformer 83, the primary 84 of which is connected to the plate circuit of tube 80. The grids 'I3 and 'i4 and the primary of a transformer 86, being inserted in the plate circuits of tubes I5 and l0, constitute a symmetric circuit 11.

The component oscillations of 1000 kc. frequency are eliminated at the outlet of filter since its primary is symmetrically connected in opposition. The resulting oscillations, Vwhich may vary in a continuous manner from 1200 to 1300 kc., are received at filter outlet 86 including a variable condenser 81 connected for example by a mechanical coupling 88 (shown in dotted line in the drawing) to variable condenser 12.

The oscillations generated by tube 80 excite also an harmonics generating tube 89 by means of its grid 90 followed by an harmonics selector QI, the movable member 92 of which allows selection at will of any of said harmonics, for example an harmonic of the order six to ten, supplying thus to grid 93 of a mixer tube 94 oscillations having a frequency of 6000, 7000, etc., up to 10,000 kc. The tube 94 is further excited on its grid 05 by the oscillations from lter 85.

The resulting oscillations in the circuit of plate 00 are separated from the component oscillations in a band passing filter 9'! (without variable condenser) wliose movable member 93 is coupled by a mechanical coupling 93 to the movable member 92. oscillations may have any value between 4700 The frequency of the resultingyl l and 4800 irc., between 5700 and 5800kc., between 6700 and 6800 kc., etc. The interval between said bands, only 100 kc. wide, allows the useof a filter 97 having no variable condenser.

The oscillations generated by the oscillating tube 80 also excite an oscillating tubeV I0! through grid tov synchronize thistubeVthe frequency of which and of oscillating circuit |02, is kept to a iixed value, for example 100 kc. The oscillating circuit |02 includes an initial adjusting condenser |03. The oscillations from the plate circuit H34v are fed to an harmonic generating tube 05 and the selection of the requiredharmonic is obtained in a filter IBB comprising two circuits coupled to critical coupling in order to obtain the maximum of, selectivity. 'Ihe movable members IGI and iS of said filter are coupled together by a mechanical linkage i639.

The oscillations from filter IGS have thus a frequency which is 800, 900 or 1700 kc. They are fed to grid H0 of a mixer il l, the other grid II2 of which is excited by the oscillations from lter 97. The resulting oscillations flow in an oscillating circuit H3 comprising a multiestep inductanoe IM, selected by a movable member f I l5, coupled by a mechanical linkage i i5 to movable members 92 and 0S. The condenser til of said` oscillating circuit is variable. .Said oscillae tions, fed to the other stages of the transmitter,

have a frequencywhich may rvary in a continuous manner, in this instance from 3000 to 8000 kc.

The following table will givethe values of the above` defined frequencies, in the considered example, to obtain oscillations of a frequency which may have any value between 3000 and 4100 kc. The table may be extended for higher values, for example up to 8000 kc., asin the selected example.

which substantially ycoincide with said wide fre-- quency band in the frequency spectrum, tuning means connected to said first oscillator for selecting one frequency from said discontinuous multiplicity, a second oscillation generator continuously variable over an interval substantially narrower than said wide band, said interval being substantially not greater than the interval between any two successive frequencies of said uniformly spaced frequencies and positioned in the frequency spectrum toward the lower limit thereof, second tuning means connected to said second oscillator, means connected to the outputs of said generators for combining the oscillations from said first and second oscillation generators to produce resultant oscillations, and a filter connected to the output of said combining means and tunable over substantially all of said wide frequency band.

2. In a system for transmitting radio frequency signals of any frequency'selected from a wide continuous frequency bandin combination: a crystal stabilized oscillation generator, a harmonics generator connected to the output of said crystal stabilized oscillator and supplying a discontinuous multiplicity of uniformly spaced frequencies having a range the limits of which substantially coincide with said wide frequency band in the frequency spectrum, a second oscillation generator continuously variable over an interval substantially narrower than said wide band, said interval being substantially not greater than the interval between any two successive frequencies of said uniformly spaced frequencies and positioned in the frequency spectrum towards the lower limit thereof, means connected to the outputs of said generators for mixing the oscillations from said second oscillation generator and said har- FlO F11 F12 F13 F15 F14 F16 300 t0 200 1,000 1,300 t0 1,200 6,000 4,700 t0 4,800 1,700 3,000 t0 3,100 300 to 200 1,000 1,300 to 1,200 6,000 4,700 to 4,800 1,000 3,100 t0 3,200 300 t0 200 1,000 1,300 to 1,200 0,000 4,700 t0 4,800 1,500 3,200 to 3,300 300 to 200 1,000 1,300 to 1,200 6,000 4,700 t0 4,800 1,400 3,300 to 3,400 300 t0 200 1,000 1,300 t0 1,200 6,000 4,700 t0 4,80n 1,300 3,400 t0 3,500 300 to 200 1,000 1,300 to 1,200 6,000 4,700 t0 4,801 1,230 3,500 to 3,600 300 to 200 1,000 1,300 t0 1,200 6,000 4,700 to 4,800 1,100 3,000 t0 3,700 300 t0 200 1,000 1,300 to 1,200 6,000 4,700 t0 4,800 1,000 3,700 to 3,800 300 to 200 1,000 1,300 to 1,200 5,000 4,700 to 4,800 900 3,800 to 3,900 300 to 200 1,000 1,300 to 1,200 6,000 4,700 t0 4,800 800 3,900 t0 4,000 300 to 200 1,000 1,300 to 1,200 7,000 5,700 t0 5,800 1,700 4,000 t0 4,100

In practice to control the frequency of the oscillations transmitted the set comprises three control members corresponding to the variations of frequency F10, of frequency Fili and of frequency FI3.

The last moves beforethe Figures 3 to 7 corresponding to thousands ofv kc., the second one moves before a 0 to 9 scale, corresponding to hundreds of kc. and thenrst one before a 0-100 scale, corresponding to kc.

YReferring now to the above .,table, it may be seen forvexainple that the Figure .3 of the thousands of kc. scale corresponds to a Value of F13 equal to 6000 kc., that the Figure 6 of the scale of thehundreds of kc. corresponds to a value of Flll equal to 1100 kc., that the Figure of the kc. dial corresponds to a value of FIG equal to 275 kc.

Weclaim:

1. In .a system for transmitting radio frequencyl signals of any frequency selected from a wide continuous frequency band, in combination: a crystal stabilized oscillation generator supplying a discontinuous multiplicity of uniformly spaced, frequencies having a range the limits of monies generator, a tunable lter connected to the output of said mixing means, a first separate control connected to said harmonics generator and said tunable filter for selecting one frequency from said discontinuous multiplicity and for tuning said filter, and a second separate control connected to said second oscillation generator and said tunable filter for simultaneously tuning said second oscillation` generator and said filter.

3. 'In a system for transmitting radio frequency signals of any frequency selectedfroma Wide continuous frequency band, in combination: a crystal stabilized oscillation generator, a harmonics generator connected to the output of said osciliw tion generator and Vsupplying a discontinuous multiplicity of uniformly spaced frequencies hav ing a range the limits of which substantially coincide with said wide frequency band in the frequency spectrum, means for selecting one of said multiplicity of uniformly spaced frequencies, a second oscillation generator continuously ivariable over a range substantially not greater than the interval between any two successive frequencies .of said y.uniformly spaced Hfrequencies, means for producing a single stabilized frequency.

first mixing means connected to the output of said second oscillation generator and to said single stabilized frequency means, second mixing means connected to the output of said first mixing means and the output of said harmonics generator, and a tunable filter connected to the output of said second mixer.

4. An apparatus as in claim 3 wherein the means for producing a single fixed frequency is stabilized by said crystal oscillator.

5. In a system for transmitting radio frequency signals of any frequency selected from a wide continuous frequency band, in combination: a iirst crystal stabilized oscillation generator supn plying a discontinuous multiplicity of uniformly spaced frequencies having a range the limits of which substantially coincide with said wide frequency band in the frequency spectrum, a second crystal stabilized oscillation generator supply'- ing a second discontinuous multiplicity of uniformly spaced frequencies having a range which substantially coincides with the interval between any two successive frequencies of said first discontinuous multiplicity and is positioned in the frequency spectrum towards the lower limit thereof, a third oscillation generator continuously variable over an interval substantially not greater in width than the interval between any two successive frequencies of said second discontinuous multiplicity and positioned in the frequency spectrum toward the lower limit thereof, a first mixer connected to the outputs of two of said three oscillation generators, a second mixer connected to the outputs of both said first mixer and the third of said oscillation generators, and a tunable filter connected to the output of said second mixer and tunable over said wide frequency band. i

6. In a system for transmitting radio frequency signals of any frequency selected from a wide continuous frequency band, in combination: a first crystal stabilized oscillation generator including a first harmonics generator supplying a discontinuous multiplicity of uniformly spaced frequencies having a range the limits of which with the interval between any two successive frequencies of said first discontinuous multiplicity and spaced in the frequency spectrum toward the lower limit thereof, second selecting means for selecting one lfrequency from said second discontinuous multiplicity of frequencies, a third oscillation generator continuously variable over an interval substantially not greater in width than the interval between any two successive frequencies of said second discontinuous multiplicity, a first mixer connected to the outputs of two of said three oscillation generators, a second mixerconnected to the outputs of said rst mixer and the other of said oscillation generators, and a filter connected to the output of said second mixer and tunable over substantially all of said wide frequency band.

7. In a system for transmitting radio frequency signals of any frequency selected from a wide continuous frequency band, in combination: a first `crystal stabilized oscillation generator in cluding a rst harmonics generator supplying u. discontinuous multiplicity of uniformly spaced frequencies having a range the limits of which substantially coincide with said wide frequency band in the frequency spectrum, iirst selecting means connected to said first harmonics generator for selecting one frequency from said discontinuous multiplicity, a second crystal stabilized oscillation generator including a second harmonies generator and supplying a second discon- I tinuous multiplicity of uniformly spaced frequencies having a range which substantially coincides with the interval between any two successive frequencies of said first discontinuous multiplicity and spaced in the frequency spectrum toward the lower limit thereof, second selecting means connected to said second harmonics generator for selecting one frequency from said second discontinuous multiplicity of frequencies, a. third oscillation generator continuously variable over an interval substantially not greater in width than the interval between any two successive frequencies of said second discontinuous multiplicity, a first mixer connected to the outputs of said second and third oscillation generators, a tunable filter connected to the output of said first mixer, a second mixer connected to the outputs of said first filter and said first oscillation generator, and a tunable filter connected to the output of said second mixer.

8, 1n a system for transmitting radio frequency signals of any frequency selected from a wide continuous frequency band, in combination: a first crystal stabilized oscillation generator including a first harmonics generator supplying a discontinuous multiplicity of uniformly spaced` frequencies having a range the limits of which substantially coincide with said wide frequency band in the frequency spectrum, first selecting means connected to said first harmonics generator for selecting one frequency from said discontinuous multiplicity, a second crystal stabilized oscillation generator including a second harmonics generator and supplying a second discontinuous multiplicity of uniformly spaced frequencies having a range which substantially coincides with the interval between any two successive frequencies of said first discontinuous multiplicity and spaced in the frequency spectrum toward the lower limit thereof, second selecting means connected to said second harmonics gencrater for selecting one frequency from said second discontinuous multiplicity of frequencies, a third oscillation generator continuously variable over an interval substantially not greater in width than the interval between any two successive frequencies of said second discontinuous multiplicity, a first mixer connected to the outputs of said second and third oscillation generators, a first tunable filter connected to the output of said first mixer, a second mixer connected to the output of said first filter and said first oscillation generator, a second tunable filter connected to the output of said second mixer, a first control connected to said third oscillation generator and said rst lter for controlling the frequencies thereof, a second control connected to said second selecting means and to said first and second filters for selecting one of said second discontinuous multiplicity of frequencies and for adjusting the pass frequencies of both of saidiilters, and a third control connected to said iirst selecting means and said second filter for selecting one of said first discontinuous multiplicity of freseremos i5 quenciesfand for adjusting'the pass frequency' of said second lter.

Y9. In a system for transmitting radio frequency signals of frequency selected ir^m a wide continuous frequency band, in com nation: a first crystal stabilized oscillation generator including a first harmonics generator supplying a discontinuous multiplicity of uniformly spaced frequencies having a range the limits of which substantially coi eide with said wide frequency ban-d in the frequency spectrum, first selecting means connected to said first harmonics generator for selecting one requency from said discontinuous multiplicity, a second crystal stabil ized oscillation generator including a second harmonics generator' and supplying a second di continuous multiplicity of uniformly spaced frequencies having a range which substantially coincides with the interval between any two sucw cessive frequencies of said first discontinuous multiplicity and spaced in the frequency spectrum toward the lower limit thereof,.second selecting means connected to said second harmonics 'gen erator for selecting one frequency from scid secon'd discontinuous multiplicity of frequencies, a third oscillation generator continuously variable over an interval substantially not greater in width than the interval'between any two successive-frequencies of said second discontinuous multiplicity, a first mixer connected 'to the outputs of said Vfirst and second oscillation generators, a first lter connected to the output of said rst'mixer, a second mixer connected to the outputs of said first filter and said third oscillation generator, and a second filter connected to the output of said second lter and tunable over substantially all of said wide freh quency band.

l0. in a system for transmitting radio frequency signals of any frequency selected from a wide continuous frequency band, in combina tion: a first crystal stabilized oscillation gencrater including a first harmonics generator supplying a discontinuous multiplicity of uniformly spaced frequencies `having a range the limits of which substantially coincide with said wide frequency band in the frequency spectrum, first selecting means connected to said first harmonics generator for selecting one frequency from said discontinuous multiplicity, a second crystal stabilized oscillation generator including a second harmonics generator and supplying a second discontinuous multiplicity of uniformly spaced frequenciesrhaving a range which substantially coincides with the interval between any two successive frequencies of said rst discontinuous multiplicity and spaced in the frequency spectrum toward the lower limit thereof, second selecting means connected to said second harmonics generator for selecting one frequency from said second discontinuous multiplicity of frequencies, a third oscillation generator continuously variable over an interval substantially not greater in width than the interval between any two successive frequencies of said second discontinuous multiplicity, a first mixer connected to the outputs of said first and third oscillation generators, a nrst lter connected to the output of said first mixer, a second mixer connected to the outputs of said first filter and said second oscillation generator, and a second nlter connected to the output of said second mixer and tunable over substantially all of said wide frequency band.

11. In a `system for transmitting radio vfrequency signals of -any frequency selected ffrom a wide continuous frequency band, in combination: a vfirst crystal stabilized oscillation gener-- ator including a first harmonics generator supplying a, discontinuous multiplicity of uniformly spaced frequencies having a range the limit-sof which substantially coincide with said widefrequency band in the frequency spectrum, rst selecting means connected to said first harmonics generator for selecting one frequency from'said discontinuous multiplicity, a second stabilized oscillation generator connected to said nrst oscil- 7ation generator and including a second harmonies generator supplying a second discontinuous multiplicity of uniformly spaced frequencies having a range which substantially coincides with the interval between any two successive frequencies of said first discontinuous multiplicityand spaced in the frequency spectrum toward the lower limit thereof, second selecting means connected to said second harmonics generator for selecting one frequency from said second discontinuous multiplicity of frequencies, a third oscillation generator continuously variable over'an interval substantially not greater in widththan the interval between any two successive frequencies of said second discontinuous multiplicity, a first mixer connected to the outputs of said first and third oscillation generators, a first filter connected to the output of said rst mixer, a second mixer connected to the outputsof said first filter and said second oscillation generator, and a second filter connected to the output of said second mixer and tunable over substantially all of said wide frequency band.

l2. In a system for transmitting radio Afrequency signals of any frequency selectedfromel wide continuous frequency band, in combination: a crystal stabilized oscillator, a first stabilized oscillator generatorv connected to said oscillator and supplying a first discontinuous multiplicity lof uniformly spaced frequencies having a range the limits of which substantially coincide with said wide'frequency band in the frequency spectrum, a first tuning element connected to said first oscillation generator for selecting one frequency from said discontinuous multiplicity of frequencies, a second stabilized oscillation generator connected to said oscillator and supplying a second discontinuous multiplicity of uniformly spaced frequencies having a range the limits of which substantially coincide with the interval between any two successive frequencies of said first discontinuous multiplicity, a second tuning element connected to said second oscillation generator for selecting one frequency from said second discontinuous multiplicity of frequencies, a third oscillaticn generator continuously variable over an interval substantially not greater than the interval between any two successive frequencies of said second multiplicity of frequencies and positioned in the frequency spectrum toward the lower limit thereof, a third tuning element connected to said third oscillation generator for adjusting the frequency of said third oscillation generator, a rst mixer connected to the outputs of both. said oscillator and said third oscillation generator, a nrst tunable filter connected to Athe output of said first mixer, a second mixer connected to the outputs of both said first tunable filter and said first oscillation generator, -a second tunable filter connected to the output of said second mixer, a third mixer connected tothe output of both said tunable filter and said second-oscillation generator, and a third tunable filter connected to the output of said third mixer.

13. In a system for transmitting radio frequency signals of any frequency selected from a wide continuous frequency band, in combination: a crystal stabilized oscillator, a first stabilized oscillation generator connected to said oscillator and including a harmonics generator for supplying a first discontinuous multiplicity of uniformly spaced frequencies having a range the limits of which substantially coincide with said Wide frequency band in the frequency spectrum, a first tuning element connected to said first oscillation generator for selecting one frequency from said discontinuous multiplicity of frequencies, a second stabilized oscillation generator connected to said oscillator including a second harmonics generator for supplying a second discontinuous multiplicity of uniformly spaced frequencies having a range the limits of which substantially coincide with the interval between any two successive frequencies of said first discontinuous multiplicity, a second tuning element connected to said second oscillation generator for selecting one-frequency from said second discontinuous multiplicity of frequencies, a third oscillation generator continuously variable over an interval substantially not greater than the interval between any two successive frequencies of said second multiplicity of frequencies and positioned in the frequency spectrum toward the lower limit thereof, a third tuning element connected to said third oscillation generator for adjusting the frequency of said third oscillation generator, a first mixer connected to the outputs of both said oscillator and said third oscillation generator, a first tunable filter connected to the output of said first mixer, a second mixer connected to the outputs of both said first tunable filter and said first oscillation generator, a second tunable filter connected to the output of said second mixer, a third mixer connected to the output of both said second tunable filter and said second oscillation generator, and a third tunable filter connected to the output of said third mixer.

14. In a system for transmitting radio frequency signals of any frequency selected from a wide continuous frequency band, in combination: a crystal stabilized oscillator, a first stabilized oscillation generator connected to said oscillator and including a first harmonics generator and selector therefor for supplying any selected frequency from a first discontinuous multiplicity of uniformly spaced frequencies having a range the limits of which substantially coincide with said Wide frequency band in the frequency spectrum, a second stabilized oscillation generator connected to said oscillator and including a second harmonics generator and selector therefor for supplying any frequency from a second discontinuous multiplicity of uniformly spaced frequencies having a range the limits of which substantially coincide with the interval between any two successive frequencies of said first multiplicty, a third oscillation generator continuously variable over an interval substantially not greater in width than the interval between any two successive frequencies of said second multiplicity and positioned in the frequency spectrum toward the lower limit thereof, a first mixer connected to the outputs of both said oscillator and said third oscillation generator, a first tunable filter connected to the output of said first mixer, a second mixer connected to the outputs of both said first tunable filter and said first oscillation generator, a second tunable filter connected to the output of said second mixer, a third mixer connected to the outputs of both said second tunable filter and said second oscillation generator, a third tunable filter connected to the output of said third mixer, a first control connected to both said third oscillation generator and said first filter for simultaneously adjusting the frequencies thereof, a second control connected to said first harmonics selector and to said second and third filters for simultaneously selecting one of said rst discontinuous multiplicity of frequencies and adjusting the pass frequencies of said filters, and a third control connected to said second harmonics selector for selecting one of said second discontinuous multiplicity of frequencies.

References Cited in the file of this patent UNITED STATES PATENTS Number Name Date 2,131,558 Granger Sept. 27, 1938 2,231,684 Monk Feb. 11, 1941 2,252,870 Slonczewski Aug. 19, 1941 2,265,083 Peterson Dec. 2, 1941 2,270,023 Ramsay et al Jan. 13, 1942 2,401,481 Harriett June 4, 1946 FOREIEGN PATENTS Number Country Date 486,448 Great Britain June 2, 1938 

